CN114674748A - High-integration photoacoustic gas sensor based on light path optimization - Google Patents
High-integration photoacoustic gas sensor based on light path optimization Download PDFInfo
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- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/01—Arrangements or apparatus for facilitating the optical investigation
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- G—PHYSICS
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- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/1702—Systems in which incident light is modified in accordance with the properties of the material investigated with opto-acoustic detection, e.g. for gases or analysing solids
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/1702—Systems in which incident light is modified in accordance with the properties of the material investigated with opto-acoustic detection, e.g. for gases or analysing solids
- G01N2021/1704—Systems in which incident light is modified in accordance with the properties of the material investigated with opto-acoustic detection, e.g. for gases or analysing solids in gases
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Abstract
The invention discloses a high-integration photoacoustic gas sensor based on optical path optimization, which comprises a substrate, a shell and a radiation source, wherein the shell and the substrate form a sealed gas chamber; a light absorption structure is arranged on the inner side wall of the shell, far away from the radiation source, in the air chamber, a plurality of cambered surface reflection structures are arranged on the inner side wall of the shell of the air chamber, the cambered surface reflection structures are distributed at the upper and lower positions of the inner side wall of the shell of the air chamber, and light emitted by the radiation source reaches the light absorption structure after being reflected by the cambered surface reflection structures; an air hole is formed in the side face of the air chamber, and a waterproof breathable film covers the air hole; a microphone, an ASIC chip and a control element are arranged on the substrate in the air chamber. The photoacoustic gas sensor disclosed by the invention realizes the purposes of miniaturization and integration, and can also improve the detection precision, the detection sensitivity and the detection limit.
Description
Technical Field
The invention relates to the field of photoacoustic measurement, in particular to a highly-integrated photoacoustic gas sensor based on optical path optimization.
Background
With the continuous development of society, the types of gases which people contact in production and life are more and more complicated, and the detection of the gas concentration has increasingly important influence on the production and life. Conventional gas detection methods include electrochemical, electrical, optical, and the like. Among them, the gas sensor based on the optical method has many advantages such as high sensitivity, good selectivity, etc.
The photoacoustic effect refers to a phenomenon that a gas absorbs modulated light to generate sound pressure, and the basic theory is that a photoacoustic signal is generated from light to heat to sound. One gas will have a strong absorption peak for light of a particular wavelength, and different gases will have strong absorption peaks for light of different wavelengths. The gas absorbs the modulated light and then undergoes a transition, the molecules that transition to the excited state release this energy in some form, and the released energy is converted into thermal energy. The gas concentration sensor based on the photoacoustic effect usually comprises four structures, namely a radiation source, a gas chamber, a sealed photoacoustic cell and a microphone. In the closed photoacoustic cell, the optical signal generated by the gas absorption modulation light source can generate a thermal signal with the same frequency, and according to an ideal gas state equation, a pressure signal with the same frequency, namely a photoacoustic signal, can be correspondingly generated. The photoacoustic signal increases with the gas concentration, and thus the concentration of the gas can be detected according to the magnitude of the photoacoustic signal.
The traditional photoacoustic gas sensor is often large in size, so that light has a long enough optical path to be absorbed by gas molecules, and the detection accuracy, sensitivity, detection limit and other indexes of the traditional photoacoustic gas sensor are guaranteed. Meanwhile, the volume of the closed photoacoustic cell is often larger and the packaging requirement is higher, so that the photoacoustic sensor is difficult to miniaturize. In addition, in the conventional photoacoustic gas sensor, the radiation source and the microphone are usually packaged separately and then packaged into the sensor again, which also results in low integration degree, complex use and high cost.
Disclosure of Invention
In order to solve the technical problems, the invention provides a highly-integrated photoacoustic gas sensor based on optical path optimization to realize a miniaturized and integrated photoacoustic gas sensor and give consideration to indexes such as detection precision, detection sensitivity and detection limit.
In order to achieve the purpose, the technical scheme of the invention is as follows:
a high-integration photoacoustic gas sensor based on optical path optimization comprises a substrate, a shell and a radiation source, wherein the shell and the substrate form a sealed gas chamber, the radiation source is arranged in the gas chamber, a plug board is vertically arranged on the substrate in the gas chamber, and the radiation source is arranged on the plug board; a light absorption structure is arranged on the inner side wall of the shell, far away from the radiation source, in the air chamber, a plurality of cambered surface reflection structures are arranged on the inner side wall of the shell of the air chamber, the cambered surface reflection structures are distributed at the upper and lower positions of the inner side wall of the shell of the air chamber, and light emitted by the radiation source reaches the light absorption structure after being reflected by the cambered surface reflection structures; the side surface of the air chamber is provided with an air hole, and a waterproof and breathable film covers the air hole; a microphone, an ASIC chip and a control element are arranged on the substrate in the air chamber.
In one technical scheme, the radiation source is an MEMS light source, is packaged in a QFN form, and is provided with a condenser lens positioned on the outer side of the MEMS light source for condensing light so as to obtain near-collimated emergent light and meet the requirement of light path design.
In another aspect, the radiation source is a laser chip.
In a further technical scheme, a light-transmitting heat insulation shell is arranged on the outer side of the radiation source, so that interference of a heat signal generated by the radiation source per se on an opto-acoustic signal is prevented.
In a further technical scheme, a shading shell is arranged on the outer side of the microphone, so that interference of light on the microphone can be shielded.
In the above scheme, the microphone and the radiation source are packaged in a bare chip form.
In the above scheme, the base plate and the insertion plate are PCB plates.
In the above scheme, the shell of the air chamber is made of metal or plastic and the inner wall of the shell is coated with a film.
In a further technical scheme, the waterproof breathable film is a molecular sieve film with a molecular screening function, can play a role in isolating interfering gases such as water vapor and the like, and can enable a gas to be detected to enter; the selective entry of different kinds of gases can also be realized.
In the above scheme, the air hole and the light absorption structure are located on the same inner side wall of the air chamber shell, so that the influence on light reflection can be reduced.
Through the technical scheme, the novel photoacoustic gas sensor based on optical path optimization has the following beneficial effects:
1. the inner side wall of the shell of the air chamber is provided with the plurality of cambered surface reflecting structures, the cambered surface reflecting structures are distributed at the upper position and the lower position of the inner side wall of the shell of the air chamber, and light emitted by the radiation source arranged on the plugboard is reflected by the plurality of cambered surface reflecting structures, so that the light can have a sufficiently long optical path and can be absorbed by gas molecules, and the detection of gas to be detected with very low concentration is facilitated.
2. The invention omits the traditional sealed photoacoustic cell, combines the air chamber and the sealed photoacoustic cell, greatly reduces the size and avoids the complex encapsulation of the sealed photoacoustic cell.
3. The radiation source and the microphone are packaged in a bare chip form and are finally packaged with the air chamber integrally, and compared with the traditional form that each part is independently packaged to form a complex system, the packaging mode provided by the invention greatly improves the integration and miniaturization degree of the sensor and reduces the process requirement.
4. Compared with the situation that the radiation source is arranged on the substrate and the light is reflected between the substrate and the top plate, the invention only needs to process the inner side wall of the shell, saves the processing procedure of the substrate independently and greatly saves the cost and the processing complexity.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings used in the description of the embodiments or the prior art will be briefly described below.
Fig. 1 is a side view of a highly integrated photoacoustic gas sensor based on optical path optimization as disclosed in embodiment 1 of the present invention;
fig. 2 is a top view of a highly integrated photoacoustic gas sensor based on optical path optimization as disclosed in embodiment 1 of the present invention;
fig. 3 is a side view of a highly integrated photoacoustic gas sensor based on optical path optimization as disclosed in embodiment 2 of the present invention;
fig. 4 is a top view of a highly integrated photoacoustic gas sensor based on optical path optimization as disclosed in embodiment 2 of the present invention.
In the figure, 1, a substrate; 2. a plugboard; 3. an air chamber; 4. air holes; 5. a waterproof breathable film; 6. a MEMS light source; 7. a condenser lens; 8. a thermally insulating enclosure; 9. a microphone; 10. an ASIC chip; 11. a control element; 12. a cambered surface reflecting structure; 13. collimating light; 14. a light absorbing structure; 15. a laser chip; 16. a housing; 17. a light-shielding housing.
Detailed Description
The technical solution in the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention.
Example 1
The invention provides a high-integration photoacoustic gas sensor based on optical path optimization, which comprises a substrate 1, a shell 16 and a radiation source, wherein the shell 16 forms a sealed gas chamber 3 with the substrate 1, and the radiation source is arranged in the gas chamber 3, as shown in figure 1. In the present embodiment, the housing 16 has a rectangular parallelepiped structure, and may have a cube, hemisphere, or the like. The substrate 1 serves to support internal components and provide electrical connections between the internal components. The shell 16 on the side surface of the air chamber 3 is provided with an air hole 4 for communicating with the external gas environment, so that the air chamber 3 is filled with the gas to be detected; the air holes 4 are covered with a waterproof and breathable film 5, and the case 16 of the air chamber 3 is connected to the substrate 1 in an airtight manner such as adhesion, thereby forming an acoustically sealed structure in the air chamber 3. The waterproof breathable film 5 can be made of materials such as polymers and the like, and is characterized by allowing the gas in the gas chamber 3 to exchange with the outside, providing acoustic sealing and keeping the pressure change.
A microphone 9, an ASIC chip 10, and a control element 11 are provided on the substrate 1 in the gas chamber 3. The ASIC chip 10 is used for controlling, pre-amplifying, etc. the signals of the microphone 9, and the control unit 11 is used for controlling the radiation source and the microphone 9. The choice of the microphone 9 is not limited to the common silicon-based microphone, silicon-based condenser microphone and other types of pressure sensors that can detect the sound pressure signal and convert it into an electrical signal, and the elements that can detect the sound pressure signal and convert it into an electrical signal are all optional, that is, the technical solution provided by the present invention is applicable to any sound transmission element. And the microphone 9 can be packaged in a bare chip form, so that the effects of simplifying the system and improving the integration level can be achieved. The outer side of the microphone is provided with a shading shell which does not influence the coupled sound and can shield the interference of light to the microphone.
The substrate 1 in the air chamber 3 is vertically provided with the plugboard 2, the plugboard 2 is arranged at a position close to one side of the air chamber 3, and the radiation source is arranged on the plugboard 2. And a light-transmitting heat insulation shell 8 is arranged outside the radiation source, so that the interference of a heat signal generated by the self-heating of the radiation source on an optical sound signal is prevented.
As shown in fig. 2, be equipped with several cambered surface reflection structure 12 on two relative casing 16 inside walls of air chamber 3, cambered surface reflection structure 12 distributes in each upper and lower position of the casing 16 inside wall of air chamber 3, set up the light that the radiation source on plugboard 2 sent, through several cambered surface reflection structure 12 between two casing 16 inside walls in whole air chamber 3, carry out multiple reflection according to the light path of design, can be so that light has enough long optical path and is absorbed by the gas molecule, be favorable to detecting the gas that awaits measuring that concentration is very low. The shell 16 of the air chamber 3 can be made of metal, the air chamber 3 with the cambered surface reflecting structure 12 on the inner side wall can be obtained by machining, then a smooth reflecting surface can be obtained by polishing, and for the metal material with low reflectivity, the reflectivity can be further increased by coating a film (gold, copper, aluminum and the like) on the surface of the metal material; or the housing 16 may be made of plastic, the air chamber 3 with the arc-shaped reflecting structure 12 on the inner wall is integrally formed by injection molding, and the smooth reflecting surface can be obtained on the formed inner wall, and at this time, the inner wall needs to be coated with a film (gold, copper, aluminum, etc.) to improve the reflectivity.
A light absorption structure 14 is arranged on the inner side wall of a shell 16 far away from the radiation source in the gas chamber 3, and the light absorption structure 14 can be a light absorption coating, such as black glue and other substances with black and rough surface characteristics; light emitted by the radiation source reaches the light absorption structure 14 after being reflected by the cambered surface reflection structures 12 and is finally absorbed by the light absorption structure 14, and the light absorption structure 14 is designed to prevent the light from being absorbed in time after being reflected for multiple times in the gas chamber 3 and influencing the detection after the next light emitting.
In this embodiment, the substrate 1 and the interposer 2 are PCB boards, such as FR4, organic polymer, aluminum substrate, etc.
In this embodiment, the microphone 9 and the radiation source are packaged in a bare chip form, so that independent packaging of each device is omitted, each device is placed in the air chamber 3, and the integration and miniaturization degree is greatly improved through integral packaging.
In this embodiment, the air holes 4 and the light absorbing structures 14 are located on the same inner sidewall of the shell 16 of the air chamber 3, so that the influence on the light reflection can be reduced.
Particularly, the waterproof breathable film can use a molecular sieve film with a molecular screening function, such as a molecular sieve film made of zeolite and the like, and is characterized in that gas with a molecular pore size larger than the pore size of a film substance cannot pass through the molecular sieve film, can play a role in isolating interference gas such as water vapor and the like, and can be communicated with an external gas environment, so that gas to be detected can enter. In addition, the selective entry of different gases can be realized by controlling the pore diameter of the molecular sieve.
Example 2
Compared with embodiment 1, this embodiment is different in that the radiation source is a laser chip 15, such as a vertical cavity surface emitting laser (vcsel), which can be integrated, as shown in fig. 3 and 4, and the design of the condenser lens 7 is not required because the laser chip 15 itself can obtain collimated light 13.
In addition, the choice of radiation source is various, and the form of the optical path design is also various, and is not limited to the shape of the housing 16 illustrated in the present invention. The radiation source capable of emitting collimated light 13 is packaged in the three-dimensional form provided by the invention, and the light path optimization design is carried out by designing the multiple reflection structure between the side walls, so that the radiation source belongs to the protection scope of the invention.
The detection principle of the photoacoustic gas sensor of the present invention is as follows:
when no gas is detected in the gas chamber 3, the optical signal generated by the radiation source is not absorbed in the gas chamber 3, so that no corresponding thermal signal is generated and no sound pressure signal is generated. When the detection gas exists in the gas chamber 3, the detection gas absorbs part of the light, so that a corresponding sound pressure signal is generated in the gas chamber 3 and is detected and output by the microphone 9. According to the photoacoustic theory, in the present embodiment, as the detection gas concentration in the external environment increases, the photoacoustic signal increases; the concentration of the detected gas can be reversely deduced according to the magnitude of the output photoacoustic signal.
The advantage of multiple reflections with optimized light path design is that the integrated photoacoustic sensor cannot detect a low target gas concentration because the housing 16 is often small in size and not optimized for light path. The optical path optimization structure designed by the invention ensures that the detection gas and the light can be fully contacted and absorbed due to multiple reflections of the light, so that the finally generated acoustic signal is more obvious.
Obviously, the photoacoustic gas sensor which is not optimally designed in a light path is difficult to miniaturize and integrate due to the limitation of detection precision, detection limit and detection sensitivity; on the contrary, the small-sized photoacoustic gas sensor has unsatisfactory detection accuracy, sensitivity, limit and other indexes. Thanks to the design of the gas chamber 3 and the three-dimensional encapsulation of the radiation source, the light is reflected for multiple times between the side walls of the gas chamber 3 to achieve the effect of optimizing the light path, and the average light path of the light in a small size is not transmitted to a large-size traditional photoacoustic sensor. The detection device realizes miniaturization and integration, and also gives consideration to indexes such as detection limit, detection sensitivity, detection precision and the like. Meanwhile, compared with the radiation source arranged on the substrate 1, the reflecting structure between the substrate 1 and the air chamber 3 is obtained by electroplating on the substrate 1, and the like, so that the processing procedure of the substrate 1 is omitted, and the cost and the processing complexity are greatly saved. Meanwhile, the air chamber 3 is manufactured by adopting an injection molding process, so that the cost is reduced. Under the same performance index, the size of the photoacoustic sensor is about 20-40% of that of the traditional photoacoustic sensor.
The previous description of the disclosed embodiments is provided to enable any person skilled in the art to make or use the present invention. Various modifications to these embodiments will be readily apparent to those skilled in the art, and the generic principles defined herein may be applied to other embodiments without departing from the spirit or scope of the invention. Thus, the present invention is not intended to be limited to the embodiments shown herein but is to be accorded the widest scope consistent with the principles and novel features disclosed herein.
Claims (10)
1. A high-integration photoacoustic gas sensor based on optical path optimization is characterized by comprising a substrate, a shell forming a sealed gas chamber with the substrate and a radiation source arranged in the gas chamber, wherein a plugboard is vertically arranged on the substrate in the gas chamber, and the radiation source is arranged on the plugboard; a light absorption structure is arranged on the inner side wall of the shell, far away from the radiation source, in the air chamber, a plurality of cambered surface reflection structures are arranged on the inner side wall of the shell of the air chamber, the cambered surface reflection structures are distributed at the upper and lower positions of the inner side wall of the shell of the air chamber, and light emitted by the radiation source reaches the light absorption structure after being reflected by the cambered surface reflection structures; the side surface of the air chamber is provided with an air hole, and a waterproof and breathable film covers the air hole; a microphone, an ASIC chip and a control element are arranged on the substrate in the air chamber.
2. The optical path optimization-based highly integrated photoacoustic gas sensor of claim 1, wherein the radiation source is a MEMS light source, which is packaged in QFN format, and a condenser lens is disposed outside the MEMS light source.
3. The highly integrated photoacoustic gas sensor based on optical path optimization of claim 1, wherein the radiation source is a laser chip.
4. A highly integrated photoacoustic gas sensor based on optical path optimization according to claim 2 or 3, wherein the radiation source is externally mounted with a light-transmissive heat-insulating enclosure.
5. The highly integrated photoacoustic gas sensor based on optical path optimization of claim 1, wherein the light-shielding housing is installed outside the microphone.
6. The highly integrated photoacoustic gas sensor based on optical path optimization of claim 1, wherein the microphone and the radiation source are packaged in a bare chip form.
7. The highly integrated photoacoustic gas sensor based on optical path optimization of claim 1, wherein the substrate and the patch board are PCB boards.
8. The highly integrated photoacoustic gas sensor based on optical path optimization of claim 1, wherein the housing of the gas chamber is made of metal or plastic and the inner wall of the gas chamber is coated with a film.
9. The highly integrated photoacoustic gas sensor based on optical path optimization of claim 1, wherein the waterproof gas permeable membrane is a molecular sieve membrane with a molecular sieving function.
10. The highly integrated photoacoustic gas sensor based on optical path optimization of claim 1, wherein the air holes and the light absorbing structures are located on the same inner sidewall of the gas cell housing.
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